Issue 30

F. Burgio et alii, Frattura ed Integrità Strutturale, 30 (2014) 68-74; DOI: 10.3221/IGF-ESIS.30.10 73 residence times and lower flow rates, 1100 °C situation, the hydrogen, flowed in the internal porosities, has sufficient time to inhibit the methane decomposition lowering the deposition rate. At 1200°C, with intermediate values of both residence time and flow rate, a compromise condition between diffusion and inhibition was established. Temperature Residence time Flow rate Deposition rate [μm/h] [°C] [s] [m/s] From Py-C thickness of the inner fibres From Py-C thickness of the outer fibres 1100 3.3 0.21 0.06 0.12 1200 3.1 0.23 0.11 0.13 1300 2.9 0.24 0.02 0.7 Table 3 : steady – state Py-C deposition rates. (a) (b) (c) Figure 8 : Optical micrographs the C f /C cross sections at (a) 1100 °C, (b) 1200 °C and (c) 1300 °C. C ONCLUSIONS he effects of CVI temperature on Py-C microstructure and infiltration behaviour have been investigated. It was found that the temperature variation in the range of 1100 to 1300 °C, at the operating condition here considered, did not affect the Py-C texture: a dark laminar Py-C was indeed obtained at all the analyzed conditions of temperature. The dark laminar texture was identified by extinction angle measurements. Raman analyses evidenced the temperature influence on microstructural order and on degree of graphitization of the obtained pyrolytic carbon: at the higher temperature (1300 °C) a more ordered and graphitized Py-C microstructure was obtained. Moreover, the process temperature affected the infiltration behaviour: at 1200 °C the Py-C infiltration resulted more homogeneous than at the other two temperatures, in terms of internal and external porosities densification. In order to obtain a dense C f /C with high mechanical properties two main features are required: an optimum value of residence time, that allows a gradual reduction of the porosities, and a Py-C matrix microstructure with high density. The results, obtained in this work, allowed to fix the residence time obtained at 1200 °C, 3.1 s, as an optimal value from the point of view of the infiltration behaviour. The change of the alfa values could lead to the obtaining of Py-C structure with higher density. R EFERENCES [1] Lopez-Honorato, E., Meadows P.J., Xiao P., Fluidized bed chemical vapor deposition of pyrolytic carbon – I. Effect of deposition conditions on microstructure, Carbon, 47 (2009) 396-410. [2] Zou, L., Huang, B., Huang, Y., Huang, Q., Wang, C., An investigation of heterogeneity of the degree of graphitization in carbon–carbon composites, Materials Chemistry and Physics, 82 (2003) 654–662. [3] Ozcan, S., Filip, P., Microstructure and wear mechanisms in C/C composites, Wear, 259 (2005) 642–650. [4] Chen, T., Gong, W., Liub, G., Zhang, F., Influence of graphite foils on I-CVI densification rate and microstructure of obtained pyrolytic carbon of carbon–carbon composites, Composites: Part A, 36 (2005) 1494–1498. T 40 µm 40 µm 40 µm